dB  Power ratio  Amplitude ratio  

100  10000000000  100000  
90  1000000000  31623  
80  100000000  10000  
70  10000000  3162  
60  1000000  1000  
50  100000  316  .2  
40  10000  100  
30  1000  31  .62  
20  100  10  
10  10  3  .162  
6  3  .981 ≈ 4  1  .995 ≈ 2 
3  1  .995 ≈ 2  1  .413 ≈ √2 
1  1  .259  1  .122 
0  1  1  
−1  0  .794  0  .891 
−3  0  .501 ≈ ^{1}⁄_{2}  0  .708 ≈ √^{1}⁄_{2} 
−6  0  .251 ≈ ^{1}⁄_{4}  0  .501 ≈ ^{1}⁄_{2} 
−10  0  .1  0  .3162 
−20  0  .01  0  .1 
−30  0  .001  0  .03162 
−40  0  .0001  0  .01 
−50  0  .00001  0  .003162 
−60  0  .000001  0  .001 
−70  0  .0000001  0  .0003162 
−80  0  .00000001  0  .0001 
−90  0  .000000001  0  .00003162 
−100  0  .0000000001  0  .00001 
An example scale showing power ratios x, amplitude ratios √x, and dB equivalents 10 log_{10} x. 
The decibel (symbol: dB) is a unit of measurement used to express the ratio of one value of a power or field quantity to another on a logarithmic scale, the logarithmic quantity being called the power level or field level, respectively. It can be used to express a change in value (e.g., +1 dB or −1 dB) or an absolute value. In the latter case, it expresses the ratio of a value to a fixed reference value; when used in this way, a suffix that indicates the reference value is often appended to the decibel symbol. For example, if the reference value is 1 volt, then the suffix is "V" (e.g., "20 dBV"), and if the reference value is one milliwatt, then the suffix is "m" (e.g., "20 dBm").^{[1]}
Two different scales are used when expressing a ratio in decibels, depending on the nature of the quantities: power and field (rootpower). When expressing a power ratio, the number of decibels is ten times its logarithm to base 10.^{[2]} That is, a change in power by a factor of 10 corresponds to a 10 dB change in level. When expressing field (rootpower) quantities, a change in amplitude by a factor of 10 corresponds to a 20 dB change in level. The decibel scales differ by a factor of two so that the related power and field levels change by the same number of decibels in, for example, resistive loads.
The definition of the decibel is based on the measurement of power in telephony of the early 20th century in the Bell System in the United States. One decibel is one tenth (deci) of one bel, named in honor of Alexander Graham Bell; however, the bel is seldom used. Today, the decibel is used for a wide variety of measurements in science and engineering, most prominently in acoustics, electronics, and control theory. In electronics, the gains of amplifiers, attenuation of signals, and signaltonoise ratios are often expressed in decibels.
In the International System of Quantities, the decibel is defined as a unit of measurement for quantities of type level or level difference, which are defined as the logarithm of the ratio of power or fieldtype quantities.^{[3]}
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✪ #22: Entenda o Decibel dB
Transcription
 [Voiceover] All right, I'm going to tell you about the Decibel Scale. This is the scale that we use to figure out the loudness of a sound. The equation that goes along with it looks like this. Beta equals 10 log, or logarithm, base 10 of I divided by 10 to the negative 12 watts per square meter. This looks intimidating. Let's talk about it and break it down. Beta is the number of decibels. So this side gives you the number of decibels and we abbreviate decibel with a little d, capital B. This is the number of dBs or decibel. You've probably seen this number on your stereo. Somewhere reader just in volume because we're going to measure volume and Decibels. 10, this 10 just denotes the fact that this is the Decibel Scale and not just the bel scale. If you didn't multiply by 10, you'd have the bel scale but this is multiplied by 10. We like the 10. We're going to call is Decibel. Log, we'll talk about log in a minute. Logarithm here. I is the intensity of the sound wave. So this is the intensity. In Physics, intensity is defined to be the power divided by the area. What this means, think about it this way. You got your ear and a sound wave, say, is coming toward your ear. If you imagine, one. Power's in, what? Power measure going to watts. Area's measure going to square meter. So think about intensity this way. If you have one square meter. Imagine one square meter of area here. This doesn't have to be an actual physical object. Just imagine a square meter of area. The power that passes through that area will be, how many jewels? If you figure you how many jewels pass through this one square meter. If you asked how many jewels per second pass through that one square meter. How many jewels of sound energy per second pass through the one square meter? That would be the number of watts per meter squared which would be the intensity. So watts is jewels per second. This gives you an idea of how much energy per second pass through a certain amount of area. This part of the equation is my favorite. This is my alltime favorite right here. This number. This 10 to the negative 12 watts per square meter represents the threshold of human hearing. What that means is this is the softest possible sound you can hear. Any sound with an intensity less than that. You won't even notice. But if it's anything bigger than that, a human ear that's healthy should be able to detect it. Here is why I like this number. This is unbelievably small. This is one trillion of a watt per meter square. A trillion. What this says is that even if only one trillionth of a jewel per second passes through the square meter, your ear would still be able to detect the sound that soft. If that doesn't impress you, let me put it to you this way. Imagine we did have one watt. Let me put it to you this way. If you have one watt, how big of an area? A watt isn't really that much. A watt is not a lot of power. If you have one watt, how big could you make this area? How, spread out. How deluded could one watt be spread over? How large of an area could this one watt be spread over and still be intense enough for the human ear to hear it? What do you think? Football field? I don't know, a city? No, it turns out. If you do the calculation, I suggest you do it. It's interesting. You would get, that you can spread one watt over the entire land area of Germany, about three times over, and still it's intense enough for the human ear to hear. That's how unbelievably sensitive our ears are. It's actually... I told you it's unbelievable. I can hardly believe it myself. Let's come back over to here. So here's our equation. This is the Decibel Scale. Why log? That's what you're thinking. "Why in God's name did the physicist have "to put logarithm in here? "This scare me." This used to scare me too. Well, I'll show you why. Here's the problem. The fact that we can hear such a soft sound, 10 to the negative 12 watts per meter squared, there's a huge range of human hearing. This means we can hear from 10 to the negative 12 watts per square meter. This is your point zero, zero, say three, four, five, six, seven, eight, nine, 10, 11, with a one watts per square meter all the way where there's no upper limit. It just blow out your ears. But once you get to about one watt per square meter, this one will start hurting. This is painful. You're not going to be happy over here. You're just going to start hurting. You'll start getting hearing losses and not good. So it's a huge range. 12 orders of magnitude. This one watt per square meter is a trillion times bigger than this side. This scale is just way too big. This is awkward. We want to scale that's small or maybe like one to 100 to measure loudness. We don't want to measure from one to a trillion or a trillion to one. That's what log's going to do. Logs are great. This is a trick for this use. This is why I love this trick. Logarithms take really big or really small numbers and turn them into nice numbers. That's why we're going to use the logarithm. Let me show you what I mean. Logarithm, if you don't remember, here's what a logarithm does. Log base 10 of a number equals, here's what it does. I'm going to stick a number in here. Let's stick 100000. What log does, log is a curious guy. Log is always asking a question. Log always wants to know, okay, if I'm log base 10, log wants to know what number would I raise 10 to in order to get this number in here. So log looks at this number in the parentheses. This entire number here and asks what number should I raise 10 to in order to get 100000. Well, we know the answer to that. We should raise 10 to the fifth. If I raise 10 to the fifth, I'll get 100000. So if five is the number I raised 10 to get 100000, then that's the answer to this that log base 10 of 100000 is five. Look what happened. Log took a huge number, 100000, and turned it into five. Well, that's outstanding. Log can take huge numbers, turn them into nice numbers. The logarithm base 10 of one billion would be... One billion is a big number. That's hard to deal with but log takes 10 and asks what number can I raise 10 to in order to get a billion. I should raise 10 to the ninth because I got one, two, three, four, five, six, seven, eight, nine zeros here. I raised 10 to the ninth to get this number. So the answer to this question for the logarithm is nine. Oops, that's not nine. Nine, and that's why logarithms are good. Logarithm took this enormous number of billion and turned it into nine. So logarithms take enormous scales turn them in nine scales. That's why we like this formula which is our Decibel Scale because it takes enormous intensities and small intensities, turns them into nice intensities. Let me show you an example with this equation really quick. Let's say you're talking to your friend. Maybe you're yelling at your friend. You guys are having a heated exchange. You're yelling. He's next to you. These are the sound waves coming at him. You're yelling with an intensity of, say 10 to the negative fifth. That doesn't sound like a lot but that's actually, you're pretty upset here. That's pretty loud. I want to know how many decibels is this. How do we figure out the decibels? Well, here's what we do. We use our formula for decibels. Beta, number of decibels, equals 10 log base 10 of the intensity over always 10 to the negative 12 watts per square meter because that's the softest sound we can hear. What do I get? 10 to the negative fifth is my intensity. So I plug this into here. I'm going to get beta equals 10 times the log base 10 of 10 to the negative fifth, because that's my intensity, divided by 10 to the negative 12. Now these are both watts per square meter. So let's cancel. Well, what's 10 to the negative fifth divided by 10 to the negative 12 turns out that's 10 to the seventh. I end up with 10 log of 10 to the seventh. Now I don't like logs. I'll be honest. They freak me out but I can even do this one. Log of 10 to the seventh. Remember what log does. It asks what number do I raise 10 to in order to get the thing in the parentheses. Well, the number I raise 10 to to get the thing in this parentheses, it's already 10 to the seventh. It's already in this form. So I've raised 10 to the seventh to get 10 to the seventh. So the answer to log base 10 of 10 to the seventh is just seven. My final answer beta, the loudness, the number of decibels is going to be 10 times log of 10 to the seventh was just seven because I have to raise 10 to the seventh to get 10 to the seventh. 10 times seven equals 70. I'm yelling at 70 decibels. I need to calm down. My friend's going to start getting mad at me. That's how you figure out how loud the sound wave is.
Contents
 1 History
 2 Definition
 3 Properties
 4 Uses
 5 Suffixes and reference values
 6 Related units
 7 Fractions
 8 See also
 9 References
 10 Further reading
 11 External links
History
The decibel originates from methods used to quantify signal loss in telegraph and telephone circuits. The unit for loss was originally Miles of Standard Cable (MSC). 1 MSC corresponded to the loss of power over a 1 mile (approximately 1.6 km) length of standard telephone cable at a frequency of 5000 radians per second (795.8 Hz), and matched closely the smallest attenuation detectable to the average listener. The standard telephone cable implied was "a cable having uniformly distributed resistance of 88 Ohms per loopmile and uniformly distributed shunt capacitance of 0.054 microfarads per mile" (approximately corresponding to 19 gauge wire).^{[4]}
In 1924, Bell Telephone Laboratories received favorable response to a new unit definition among members of the International Advisory Committee on Long Distance Telephony in Europe and replaced the MSC with the Transmission Unit (TU). 1 TU was defined such that the number of TUs was ten times the base10 logarithm of the ratio of measured power to a reference power.^{[5]} The definition was conveniently chosen such that 1 TU approximated 1 MSC; specifically, 1 MSC was 1.056 TU. In 1928, the Bell system renamed the TU into the decibel,^{[6]} being one tenth of a newly defined unit for the base10 logarithm of the power ratio. It was named the bel, in honor of the telecommunications pioneer Alexander Graham Bell.^{[7]} The bel is seldom used, as the decibel was the proposed working unit.^{[8]}
The naming and early definition of the decibel is described in the NBS Standard's Yearbook of 1931:^{[9]}
Since the earliest days of the telephone, the need for a unit in which to measure the transmission efficiency of telephone facilities has been recognized. The introduction of cable in 1896 afforded a stable basis for a convenient unit and the "mile of standard" cable came into general use shortly thereafter. This unit was employed up to 1923 when a new unit was adopted as being more suitable for modern telephone work. The new transmission unit is widely used among the foreign telephone organizations and recently it was termed the "decibel" at the suggestion of the International Advisory Committee on Long Distance Telephony.
The decibel may be defined by the statement that two amounts of power differ by 1 decibel when they are in the ratio of 10^{0.1} and any two amounts of power differ by N decibels when they are in the ratio of 10^{N(0.1)}. The number of transmission units expressing the ratio of any two powers is therefore ten times the common logarithm of that ratio. This method of designating the gain or loss of power in telephone circuits permits direct addition or subtraction of the units expressing the efficiency of different parts of the circuit ...
In 1954, J. W. Horton argued that the use of the decibel as a unit for quantities other than transmission loss led to confusion, and suggested the name 'logit' for "standard magnitudes which combine by addition".^{[10]}^{[clarification needed]}
In April 2003, the International Committee for Weights and Measures (CIPM) considered a recommendation for the inclusion of the decibel in the International System of Units (SI), but decided against the proposal.^{[11]} However, the decibel is recognized by other international bodies such as the International Electrotechnical Commission (IEC) and International Organization for Standardization (ISO).^{[12]} The IEC permits the use of the decibel with field quantities as well as power and this recommendation is followed by many national standards bodies, such as NIST, which justifies the use of the decibel for voltage ratios.^{[13]} The term field quantity is deprecated by ISO 800001, which favors rootpower. In spite of their widespread use, suffixes (such as in dBA or dBV) are not recognized by the IEC or ISO.
Definition
ISO 800003 describes definitions for quantities and units of space and time. The decibel for use in acoustics is defined in ISO 800008. The major difference from the article below is that for acoustics the decibel has no absolute value.
The ISO Standard 800003:2006 defines the following quantities. The decibel (dB) is onetenth of a bel: 1 dB = 0.1 B. The bel (B) is ^{1}⁄_{2} ln(10) nepers: 1 B = ^{1}⁄_{2} ln(10) Np. The neper is the change in the level of a field quantity when the field quantity changes by a factor of e, that is 1 Np = ln(e) = 1, thereby relating all of the units as nondimensional natural log of fieldquantity ratios, 1 dB = 0.11513… Np = 0.11513…. Finally, the level of a quantity is the logarithm of the ratio of the value of that quantity to a reference value of the same kind of quantity.
Therefore, the bel represents the logarithm of a ratio between two power quantities of 10:1, or the logarithm of a ratio between two field quantities of √10:1.^{[14]}
Two signals whose levels differ by one decibel have a power ratio of 10^{1/10}, which is approximately 1.25893, and an amplitude (field quantity) ratio of 10^{1⁄20} (1.12202).^{[15]}^{[16]}
The bel is rarely used either without a prefix or with SI unit prefixes other than deci; it is preferred, for example, to use hundredths of a decibel rather than millibels. Thus, five onethousandths of a bel would normally be written '0.05 dB', and not '5 mB'.^{[17]}
The method of expressing a ratio as a level in decibels depends on whether the measured property is a power quantity or a rootpower quantity; see Field, power, and rootpower quantities for details.
Power quantities
When referring to measurements of power quantities, a ratio can be expressed as a level in decibels by evaluating ten times the base10 logarithm of the ratio of the measured quantity to reference value. Thus, the ratio of P (measured power) to P_{0} (reference power) is represented by L_{P}, that ratio expressed in decibels,^{[18]} which is calculated using the formula:^{[3]}
The base10 logarithm of the ratio of the two power quantities is the number of bels. The number of decibels is ten times the number of bels (equivalently, a decibel is onetenth of a bel). P and P_{0} must measure the same type of quantity, and have the same units before calculating the ratio. If P = P_{0} in the above equation, then L_{P} = 0. If P is greater than P_{0} then L_{P} is positive; if P is less than P_{0} then L_{P} is negative.
Rearranging the above equation gives the following formula for P in terms of P_{0} and L_{P}:
Field quantities and rootpower quantities
When referring to measurements of field quantities, it is usual to consider the ratio of the squares of F (measured field) and F_{0} (reference field). This is because in most applications power is proportional to the square of field, and historically their definitions were formulated to give the same value for relative ratios in such typical cases. Thus, the following definition is used:
The formula may be rearranged to give
Similarly, in electrical circuits, dissipated power is typically proportional to the square of voltage or current when the impedance is constant. Taking voltage as an example, this leads to the equation for power gain level L_{G}:
where V_{out} is the rootmeansquare (rms) output voltage, V_{in} is the rms input voltage. A similar formula holds for current.
The term rootpower quantity is introduced by ISO Standard 800001:2009 as a substitute of field quantity. The term field quantity is deprecated by that standard.
Relationship between power level and field level
Although power and field quantities are different quantities, their respective levels are historically measured in the same units, typically decibels. A factor of 2 is introduced to make changes in the respective levels match under restricted conditions such as when the medium is linear and the same waveform is under consideration with changes in amplitude, or the medium impedance is linear and independent of both frequency and time. This relies on the relationship
holding.^{[19]} In a nonlinear system, this relationship will not hold by the definition of linearity. However, even in a linear system in which the power quantity is the product of two linearly related quantities (e.g. voltage and current), if the impedance is frequency or timedependent, this relationhip will not hold in general, for example if the energy spectrum of the waveform changes.
For differences in level, the required relationship is relaxed from that above to one of proportionality (i.e., the reference quantities P_{0} and F_{0} need not be related), or equivalently,
must hold to allow the power level difference to be equal to the field level difference from power P_{1} and V_{1} to P_{2} and V_{2}. An example might be an amplifier with unity voltage gain independent of load and frequency driving a load with a frequencydependent impedance: the relative voltage gain of the amplifier is always 0 dB, but the power gain depends on the changing spectral composition of the waveform being amplified. Frequencydependent impedances may be analyzed by considering the quantities power spectral density and the associated field quantities via the Fourier transform, which allows elimination of the frequency dependence in the analysis by analyzing the system at each frequency independently.
Conversions
Since logarithm differences measured in these units are used to represent power ratios and field ratios, the values of the ratios represented by each unit are also included in the table.
Unit  In decibels  In bels  In nepers  Power ratio  Field ratio 

1 dB  1 dB  0.1 B  0.11513 Np  10^{1⁄10} ≈ 1.25893  10^{1⁄20} ≈ 1.12202 
1 Np  8.68589 dB  0.868589 B  1 Np  e^{2} ≈ 7.38906  e ≈ 2.71828 
1 B  10 dB  1 B  1.1513 Np  10  10^{1⁄2} ≈ 3.16228 
Examples
The unit dBW is often used to denote a ratio for which the reference is 1 W, and similarly dBm for a 1 mW reference point.
 Calculating the ratio of 1 kW (one kilowatt, or 1000 watts) to 1 W in decibels yields:
 The ratio of √1000 V ≈ 31.62 V to 1 V in decibels is
(31.62 V / 1 V)^{2} ≈ 1 kW / 1 W, illustrating the consequence from the definitions above that L_{G} has the same value, 30 dB, regardless of whether it is obtained from powers or from amplitudes, provided that in the specific system being considered power ratios are equal to amplitude ratios squared.
 The ratio of 1 mW (one milliwatt) to 10 W in decibels is obtained with the formula
 The power ratio corresponding to a 3 dB change in level is given by
A change in power ratio by a factor of 10 corresponds to a change in level of 10 dB. A change in power ratio by a factor of 2 or ^{1}⁄_{2} is approximately a change of 3 dB. More precisely, the change is ±3.0103 dB, but this is almost universally rounded to "3 dB" in technical writing. This implies an increase in voltage by a factor of √2 ≈ 1.4142. Likewise, a doubling or halving of the voltage, and quadrupling or quartering of the power, is commonly described as "6 dB" rather than ±6.0206 dB.
Should it be necessary to make the distinction, the number of decibels is written with additional significant figures. 3.000 dB is a power ratio of 10^{3⁄10}, or 1.9953, about 0.24% different from exactly 2, and a voltage ratio of 1.4125, 0.12% different from exactly √2. Similarly, an increase of 6.000 dB is the power ratio is 10^{6⁄10} ≈ 3.9811, about 0.5% different from 4.
Properties
The decibel is useful for representing large ratios and for simplifying representation of multiplied effects such as attenuation from multiple sources along a signal chain. Its application in systems with additive effects is less intuitive.
Reporting large ratios
The logarithmic scale nature of the decibel means that a very large range of ratios can be represented by a convenient number, in a manner similar to scientific notation. This allows one to clearly visualize huge changes of some quantity. See Bode plot and Semilog plot. For example, 120 dB SPL may be clearer than "a trillion times more intense than the threshold of hearing".
Representation of multiplication operations
Level values in decibels can be added instead of multiplying the underlying power values, which means that the overall gain of a multicomponent system, such as a series of amplifier stages, can be calculated by summing the gains in decibels of the individual components, rather than multiply the amplification factors; that is, log(A × B × C) = log(A) + log(B) + log(C). Practically, this means that, armed only with the knowledge that 1 dB is a power gain of approximately 26%, 3 dB is approximately 2× power gain, and 10 dB is 10× power gain, it is possible to determine the power ratio of a system from the gain in dB with only simple addition and multiplication. For example:
 A system consists of 3 amplifiers in series, with gains (ratio of power out to in) of 10 dB, 8 dB, and 7 dB respectively, for a total gain of 25 dB. Broken into combinations of 10, 3, and 1 dB, this is:
 25 dB = 10 dB + 10 dB + 3 dB + 1 dB + 1 dB
 With an input of 1 watt, the output is approximately
 1 W × 10 × 10 × 2 × 1.26 × 1.26 ≈ 317.5 W
 Calculated exactly, the output is 1 W × 10^{25⁄10} = 316.2 W. The approximate value has an error of only +0.4% with respect to the actual value, which is negligible given the precision of the values supplied and the accuracy of most measurement instrumentation.
 A system consists of 3 amplifiers in series, with gains (ratio of power out to in) of 10 dB, 8 dB, and 7 dB respectively, for a total gain of 25 dB. Broken into combinations of 10, 3, and 1 dB, this is:
However, according to its critics, the decibel creates confusion, obscures reasoning, is more related to the era of slide rules than to modern digital processing, and is cumbersome and difficult to interpret.^{[20]}
Representation of addition operations
According to Mitschke,^{[21]} "The advantage of using a logarithmic measure is that in a transmission chain, there are many elements concatenated, and each has its own gain or attenuation. To obtain the total, addition of decibel values is much more convenient than multiplication of the individual factors." However, for the same reason that humans excel at additive operation over multiplication, decibels are awkward in inherently additive operations:^{[22]} "if two machines each individually produce a sound pressure level of, say, 90 dB at a certain point, then when both are operating together we should expect the combined sound pressure level to increase to 93 dB, but certainly not to 180 dB!"; "suppose that the noise from a machine is measured (including the contribution of background noise) and found to be 87 dBA but when the machine is switched off the background noise alone is measured as 83 dBA. [...] the machine noise [level (alone)] may be obtained by 'subtracting' the 83 dBA background noise from the combined level of 87 dBA; i.e., 84.8 dBA."; "in order to find a representative value of the sound level in a room a number of measurements are taken at different positions within the room, and an average value is calculated. [...] Compare the logarithmic and arithmetic averages of [...] 70 dB and 90 dB: logarithmic average = 87 dB; arithmetic average = 80 dB."
Addition on a logarithmic scale is called logarithmic addition, and can be defined by taking exponentials to convert to a linear scale, adding there, and then taking logarithms to return. For example, where operations on decibels are logarithmic addition/subtraction and logarithmic multiplication/division, while operations on the linear scale are the usual operations:
Note that the logarithmic mean is obtained from the logarithmic sum by subtracting , since logarithmic division is linear subtraction.
Quantities in decibels are not necessarily additive,^{[23]}^{[24]} thus being "of unacceptable form for use in dimensional analysis".^{[25]}^{[clarification needed]}
Uses
Perception
The human perception of the intensity of sound and light approximates the logarithm of intensity rather than a linear relationship (Weber–Fechner law), making the dB scale a useful measure.^{[26]}^{[27]}^{[28]}^{[29]}^{[30]}^{[31]}
Acoustics
The decibel is commonly used in acoustics as a unit of sound pressure level. The reference pressure for sound in air is set at the typical threshold of perception of an average human and there are common comparisons used to illustrate different levels of sound pressure. Sound pressure is a field quantity, therefore the field version of the unit definition is used:
where p_{rms} is the root mean square of the measured sound pressure and p_{ref} is the standard reference sound pressure of 20 micropascals in air or 1 micropascal in water.^{[32]}
Use of the decibel in underwater acoustics leads to confusion, in part because of this difference in reference value.^{[33]}
The human ear has a large dynamic range in sound reception. The ratio of the sound intensity that causes permanent damage during short exposure to that of the quietest sound that the ear can hear is greater than or equal to 1 trillion (10^{12}).^{[34]} Such large measurement ranges are conveniently expressed in logarithmic scale: the base10 logarithm of 10^{12} is 12, which is expressed as a sound pressure level of 120 dB re 20 μPa.
Since the human ear is not equally sensitive to all sound frequencies, noise levels at maximum human sensitivity, somewhere between 2 and 4 kHz, are factored more heavily into some measurements using frequency weighting. (See also Stevens' power law.)
The main instrument used for measuring sound levels in the environment and in the workplace is the Sound Level Meter. Most sound level meters provide readings in A, C, and Zweighted decibels and must meet international standards such as IEC 616722013.
According to Hickling, "Decibels are a useless affectation, which is impeding the development of noise control as an engineering discipline."^{[20]}
Electronics
In electronics, the decibel is often used to express power or amplitude ratios (as for gains) in preference to arithmetic ratios or percentages. One advantage is that the total decibel gain of a series of components (such as amplifiers and attenuators) can be calculated simply by summing the decibel gains of the individual components. Similarly, in telecommunications, decibels denote signal gain or loss from a transmitter to a receiver through some medium (free space, waveguide, coaxial cable, fiber optics, etc.) using a link budget.
The decibel unit can also be combined with a reference level, often indicated via a suffix, to create an absolute unit of electric power. For example, it can be combined with "m" for "milliwatt" to produce the "dBm". A power level of 0 dBm corresponds to one milliwatt, and 1 dBm is one decibel greater (about 1.259 mW).
In professional audio specifications, a popular unit is the dBu. This is relative to the root mean square voltage which delivers 1 mW (0 dBm) into a 600ohm resistor, or √1 mW×600 Ω ≈ 0.775 V_{RMS}. When used in a 600ohm circuit (historically, the standard reference impedance in telephone circuits), dBu and dBm are identical.
Optics
In an optical link, if a known amount of optical power, in dBm (referenced to 1 mW), is launched into a fiber, and the losses, in dB (decibels), of each component (e.g., connectors, splices, and lengths of fiber) are known, the overall link loss may be quickly calculated by addition and subtraction of decibel quantities.^{[35]}
In spectrometry and optics, the blocking unit used to measure optical density is equivalent to −1 B.
Video and digital imaging
In connection with video and digital image sensors, decibels generally represent ratios of video voltages or digitized light intensities, using 20 log of the ratio, even when the represented intensity (optical power) is directly proportional to the voltage generated by the sensor, not to its square, as in a CCD imager where response voltage is linear in intensity.^{[36]} Thus, a camera signaltonoise ratio or dynamic range quoted as 40 dB represents a ratio of 100:1 between signal intensity and noise intensity, not 10,000:1.^{[37]} Sometimes the 20 log ratio definition is applied to electron counts or photon counts directly, which are proportional to sensor signal amplitude without the need to consider whether the voltage response to intensity is linear.^{[38]}
However, as mentioned above, the 10 log intensity convention prevails more generally in physical optics, including fiber optics, so the terminology can become murky between the conventions of digital photographic technology and physics. Most commonly, quantities called "dynamic range" or "signaltonoise" (of the camera) would be specified in 20 log dB, but in related contexts (e.g. attenuation, gain, intensifier SNR, or rejection ratio) the term should be interpreted cautiously, as confusion of the two units can result in very large misunderstandings of the value.
Photographers typically use an alternative base2 log unit, the stop, to describe light intensity ratios or dynamic range.
Suffixes and reference values
Suffixes are commonly attached to the basic dB unit in order to indicate the reference value by which the ratio is calculated. For example, dBm indicates power measurement relative to 1 milliwatt.
In cases where the unit value of the reference is stated, the decibel value is known as "absolute". If the unit value of the reference is not explicitly stated, as in the dB gain of an amplifier, then the decibel value is considered relative.
The SI does not permit attaching qualifiers to units, whether as suffix or prefix, other than standard SI prefixes. Therefore, even though the decibel is accepted for use alongside SI units, the practice of attaching a suffix to the basic dB unit, forming compound units such as dBm, dBu, dBA, etc., is not.^{[13]} The proper way, according to the IEC 600273,^{[12]} is either as L_{x} (re x_{ref}) or as L_{x/xref}, where x is the quantity symbol and x_{ref} is the value of the reference quantity, e.g., L_{E} (re 1 μV/m) = L_{E/(1 μV/m)} for the electric field strength E relative to 1 μV/m reference value.
Outside of documents adhering to SI units, the practice is very common as illustrated by the following examples. There is no general rule, with various disciplinespecific practices. Sometimes the suffix is a unit symbol ("W","K","m"), sometimes it is a transliteration of a unit symbol ("uV" instead of μV for microvolt), sometimes it is an acronym for the unit's name ("sm" for square meter, "m" for milliwatt), other times it is a mnemonic for the type of quantity being calculated ("i" for antenna gain with respect to an isotropic antenna, "λ" for anything normalized by the EM wavelength), or otherwise a general attribute or identifier about the nature of the quantity ("A" for Aweighted sound pressure level). The suffix is often connected with a dash (dBHz), with a space (dB HL), with no intervening character (dBm), or enclosed in parentheses (dB(sm)).
Voltage
Since the decibel is defined with respect to power, not amplitude, conversions of voltage ratios to decibels must square the amplitude, or use the factor of 20 instead of 10, as discussed above.
 dBV
 dB(V_{RMS}) – voltage relative to 1 volt, regardless of impedance.^{[1]} This is used to measure microphone sensitivity, and also to specify the consumer linelevel of −10 dBV, in order to reduce manufacturing costs relative to equipment using a +4 dBu linelevel signal.^{[39]}
 dBu or dBv
 RMS voltage relative to . An RMS voltage of 1 V is therefore corresponds to ^{[1]} Originally dBv, it was changed to dBu to avoid confusion with dBV.^{[40]} The "v" comes from "volt", while "u" comes from the volume unit used in the VU meter.^{[41]} dBu can be used as a measure of voltage, regardless of impedance, but is derived from a 600 Ω load dissipating 0 dBm (1 mW). The reference voltage comes from the computation . In professional audio, equipment may be calibrated to indicate a "0" on the VU meters some finite time after a signal has been applied at an amplitude of +4 dBu. Consumer equipment typically uses a lower "nominal" signal level of −10 dBV.^{[42]} Therefore, many devices offer dual voltage operation (with different gain or "trim" settings) for interoperability reasons. A switch or adjustment that covers at least the range between +4 dBu and −10 dBV is common in professional equipment.
 dBu0s
 Defined by Recommendation ITUR V.574.
 dBm0s
 Defined by Recommendation ITUR V.574.; dBmV: dB(mV_{RMS}) – voltage relative to 1 millivolt across 75 Ω.^{[43]} Widely used in cable television networks, where the nominal strength of a single TV signal at the receiver terminals is about 0 dBmV. Cable TV uses 75 Ω coaxial cable, so 0 dBmV corresponds to −78.75 dBW (−48.75 dBm) or approximately 13 nW.
 dBμV or dBuV
 dB(μV_{RMS}) – voltage relative to 1 microvolt. Widely used in television and aerial amplifier specifications. 60 dBμV = 0 dBmV.
Acoustics
Probably the most common usage of "decibels" in reference to sound level is dB SPL, sound pressure level referenced to the nominal threshold of human hearing:^{[44]} The measures of pressure (a field quantity) use the factor of 20, and the measures of power (e.g. dB SIL and dB SWL) use the factor of 10.
 dB SPL
 dB SPL (sound pressure level) – for sound in air and other gases, relative to 20 micropascals (μPa) = ×10^{−5} Pa, approximately the quietest sound a human can hear. For 2sound in water and other liquids, a reference pressure of 1 μPa is used.^{[45]} An RMS sound pressure of one pascal corresponds to a level of 94 dB SPL.
 dB SIL
 dB sound intensity level – relative to 10^{−12} W/m^{2}, which is roughly the threshold of human hearing in air.
 dB SWL
 dB sound power level – relative to 10^{−12} W.
 dBA, dBB, and dBC
 These symbols are often used to denote the use of different weighting filters, used to approximate the human ear's response to sound, although the measurement is still in dB (SPL). These measurements usually refer to noise and its effects on humans and other animals, and they are widely used in industry while discussing noise control issues, regulations and environmental standards. Other variations that may be seen are dB_{A} or dB(A). According to ANSI standards,^{[46]} the preferred usage is to write L_{A} = x dB. Nevertheless, the units dBA and dB(A) are still commonly used as a shorthand for Aweighted measurements. Compare dBc, used in telecommunications.
 dB HL
 dB hearing level is used in audiograms as a measure of hearing loss. The reference level varies with frequency according to a minimum audibility curve as defined in ANSI and other standards, such that the resulting audiogram shows deviation from what is regarded as 'normal' hearing.^{[citation needed]}
 dB Q
 sometimes used to denote weighted noise level, commonly using the ITUR 468 noise weighting^{[citation needed]}
 dBpp
 relative to the peak to peak sound pressure.^{[47]}
 dBG
 Gweighted spectrum ^{[48]}
Audio electronics
See also dBV and dBu above.
 dBm
 dB(mW) – power relative to 1 milliwatt. In audio and telephony, dBm is typically referenced relative to a 600 ohm impedance,^{[49]} which corresponds to a voltage level of 0.775 volts or 775 millivolts.
 dBFS
 dB(full scale) – the amplitude of a signal compared with the maximum which a device can handle before clipping occurs. Fullscale may be defined as the power level of a fullscale sinusoid or alternatively a fullscale square wave. A signal measured with reference to a fullscale sinewave will appear 3 dB weaker when referenced to a fullscale square wave, thus: 0 dBFS(fullscale sine wave) = −3 dBFS(fullscale square wave).
 dBVU
 dB volume unit^{[50]}
 dBTP
 dB(true peak) – peak amplitude of a signal compared with the maximum which a device can handle before clipping occurs.^{[51]} In digital systems, 0 dBTP would equal the highest level (number) the processor is capable of representing. Measured values are always negative or zero, since they are less than or equal to fullscale.
 dBm0
 Power in dBm measured at a zero transmission level point.
Radar
 dBZ
 dB(Z) – decibel relative to Z = 1 mm^{6}⋅m^{−3}:^{[52]} energy of reflectivity (weather radar), related to the amount of transmitted power returned to the radar receiver. Values above 15–20 dBZ usually indicate falling precipitation.^{[53]}
 dBsm
 dB(m^{2}) – decibel relative to one square meter: measure of the radar cross section (RCS) of a target. The power reflected by the target is proportional to its RCS. "Stealth" aircraft and insects have negative RCS measured in dBsm, large flat plates or nonstealthy aircraft have positive values.^{[54]}
Radio power, energy, and field strength
 dBc
 relative to carrier – in telecommunications, this indicates the relative levels of noise or sideband power, compared with the carrier power. Compare dBC, used in acoustics.
 dBpp
 relative to the maximum value of the peak power.
 dBJ
 energy relative to 1 joule. 1 joule = 1 watt second = 1 watt per hertz, so power spectral density can be expressed in dBJ.
 dBm
 dB(mW) – power relative to 1 milliwatt. In the radio field, dBm is usually referenced to a 50 ohm load, with the resultant voltage being 0.224 volts.^{[55]}
 dBμV/m, dBuV/m, or dBμ
 ^{[56]} dB(μV/m) – electric field strength relative to 1 microvolt per meter. Often used to specify the signal strength from a television broadcast at a receiving site (the signal measured at the antenna output will be in dBμV).
 dBf
 dB(fW) – power relative to 1 femtowatt.
 dBW
 dB(W) – power relative to 1 watt.
 dBk
 dB(kW) – power relative to 1 kilowatt.
 dBe
 dB electrical.
 dBo
 dB optical. A change of 1 dBo in optical power can result in a change of up to 2 dBe in electrical signal power in system that is thermal noise limited.^{[57]}
Antenna measurements
 dBi
 dB(isotropic) – the forward gain of an antenna compared with the hypothetical isotropic antenna, which uniformly distributes energy in all directions. Linear polarization of the EM field is assumed unless noted otherwise.
 dBd
 dB(dipole) – the forward gain of an antenna compared with a halfwave dipole antenna. 0 dBd = 2.15 dBi
 dBiC
 dB(isotropic circular) – the forward gain of an antenna compared to a circularly polarized isotropic antenna. There is no fixed conversion rule between dBiC and dBi, as it depends on the receiving antenna and the field polarization.
 dBq
 dB(quarterwave) – the forward gain of an antenna compared to a quarter wavelength whip. Rarely used, except in some marketing material. 0 dBq = −0.85 dBi
 dBsm
 dB(m^{2}) – decibel relative to one square meter: measure of the antenna effective area.^{[58]}
 dBm^{−1}
 dB(m^{−1}) – decibel relative to reciprocal of meter: measure of the antenna factor.
Other measurements
 dBHz
 dB(Hz) – bandwidth relative to one hertz. E.g., 20 dBHz corresponds to a bandwidth of 100 Hz. Commonly used in link budget calculations. Also used in carriertonoisedensity ratio (not to be confused with carriertonoise ratio, in dB).
 dBov or dBO
 dB(overload) – the amplitude of a signal (usually audio) compared with the maximum which a device can handle before clipping occurs. Similar to dBFS, but also applicable to analog systems. According to ITUT Rec. G.100.1 the Level in dBov of a digital system is defined as:: , with the maximum signal power , for a rectangular signal with the maximum amplitude . The level of a tone with a digital amplitude (peak value) of is therefore .^{[59]}
 dBr
 dB(relative) – simply a relative difference from something else, which is made apparent in context. The difference of a filter's response to nominal levels, for instance.
 dBrn
 dB above reference noise. See also dBrnC
 dBrnC
 dBrnC represents an audio level measurement, typically in a telephone circuit, relative to the circuit noise level, with the measurement of this level frequencyweighted by a standard Cmessage weighting filter. The Cmessage weighting filter was chiefly used in North America. The Psophometric filter is used for this purpose on international circuits. See Psophometric weighting to see a comparison of frequency response curves for the Cmessage weighting and Psophometric weighting filters.^{[60]}
 dBK
 dB(K) – decibels relative to 1 K: Used to express noise temperature.^{[61]}
 dB/K
 dB(K^{−1}) – decibels relative to 1 K^{−1}.^{[62]}—not decibels per kelvin: Used for the G/T factor, a figure of merit utilized in satellite communications, relating the antenna gain G to the receiver system noise equivalent temperature T.^{[63]}^{[64]}
List of suffixes in alphabetical order
Unpunctuated suffixes
 dBA
 see dB(A).
 dBB
 see dB(B).
 dBc
 relative to carrier – in telecommunications, this indicates the relative levels of noise or sideband power, compared with the carrier power.
 dBC
 see dB(C).
 dBd
 dB(dipole) – the forward gain of an antenna compared with a halfwave dipole antenna. 0 dBd = 2.15 dBi
 dBe
 dB electrical.
 dBf
 dB(fW) – power relative to 1 femtowatt.
 dBFS
 dB(full scale) – the amplitude of a signal compared with the maximum which a device can handle before clipping occurs. Fullscale may be defined as the power level of a fullscale sinusoid or alternatively a fullscale square wave. A signal measured with reference to a fullscale sinewave will appear 3 dB weaker when referenced to a fullscale square wave, thus: 0 dBFS(fullscale sine wave) = −3 dBFS(fullscale square wave).
 dBG
 Gweighted spectrum
 dBi
 dB(isotropic) – the forward gain of an antenna compared with the hypothetical isotropic antenna, which uniformly distributes energy in all directions. Linear polarization of the EM field is assumed unless noted otherwise.
 dBiC
 dB(isotropic circular) – the forward gain of an antenna compared to a circularly polarized isotropic antenna. There is no fixed conversion rule between dBiC and dBi, as it depends on the receiving antenna and the field polarization.
 dBJ
 energy relative to 1 joule. 1 joule = 1 watt second = 1 watt per hertz, so power spectral density can be expressed in dBJ.
 dBk
 dB(kW) – power relative to 1 kilowatt.
 dBK
 dB(K) – decibels relative to kelvin: Used to express noise temperature.
 dBm
 dB(mW) – power relative to 1 milliwatt.
 dBm0
 Power in dBm measured at a zero transmission level point.
 dBm0s
 Defined by Recommendation ITUR V.574.
 dBmV
 dB(mV_{RMS}) – voltage relative to 1 millivolt across 75 Ω.
 dBo
 dB optical. A change of 1 dBo in optical power can result in a change of up to 2 dBe in electrical signal power in system that is thermal noise limited.
 dBO
 see dBov
 dBov or dBO
 dB(overload) – the amplitude of a signal (usually audio) compared with the maximum which a device can handle before clipping occurs.
 dBpp
 relative to the peak to peak sound pressure.
 dBpp
 relative to the maximum value of the peak power.
 dBq
 dB(quarterwave) – the forward gain of an antenna compared to a quarter wavelength whip. Rarely used, except in some marketing material. 0 dBq = −0.85 dBi
 dBr
 dB(relative) – simply a relative difference from something else, which is made apparent in context. The difference of a filter's response to nominal levels, for instance.
 dBrn
 dB above reference noise. See also dBrnC
 dBrnC
 dBrnC represents an audio level measurement, typically in a telephone circuit, relative to the circuit noise level, with the measurement of this level frequencyweighted by a standard Cmessage weighting filter. The Cmessage weighting filter was chiefly used in North America.
 dBsm
 dB(m^{2}) – decibel relative to one square meter
 dBTP
 dB(true peak) – peak amplitude of a signal compared with the maximum which a device can handle before clipping occurs.
 dBu or dBv
 RMS voltage relative to .
 dBu0s
 Defined by Recommendation ITUR V.574.
 dBuV
 see dBμV
 dBuV/m
 see dBμV/m
 dBv
 see dBu
 dBV
 dB(V_{RMS}) – voltage relative to 1 volt, regardless of impedance.
 dBVU
 dB volume unit
 dBW
 dB(W) – power relative to 1 watt.
 dBZ
 dB(Z) – decibel relative to Z = 1 mm^{6}⋅m^{−3}
 dBμ
 see dBμV/m
 dBμV or dBuV
 dB(μV_{RMS}) – voltage relative to 1 microvolt.
 dBμV/m, dBuV/m, or dBμ
 dB(μV/m) – electric field strength relative to 1 microvolt per meter.
Suffixes preceded by a space
 dB HL
 dB hearing level is used in audiograms as a measure of hearing loss.
 dB Q
 sometimes used to denote weighted noise level
 dB SIL
 dB sound intensity level – relative to 10^{−12} W/m^{2}
 dB SPL
 dB SPL (sound pressure level) – for sound in air and other gases, relative to 20 μPa in air or 1 μPa in water
 dB SWL
 dB sound power level – relative to 10^{−12} W.
Suffixes within parentheses
 dB(A), dB(B), and dB(C)
 These symbols are often used to denote the use of different weighting filters, used to approximate the human ear's response to sound, although the measurement is still in dB (SPL). These measurements usually refer to noise and its effects on humans and other animals, and they are widely used in industry while discussing noise control issues, regulations and environmental standards. Other variations that may be seen are dB_{A} or dBA.
Other suffixes
 dBHz
 dB(Hz) – bandwidth relative to one hertz.
 dB/K
 dB(K^{−1}) – decibels relative to reciprocal of kelvin
 dBm^{−1}
 dB(m^{−1}) – decibel relative to reciprocal of meter: measure of the antenna factor.
Related units
 mBm
 mB(mW) – power relative to 1 milliwatt, in millibels (one hundredth of a decibel). 100 mBm = 1 dBm. This unit is in the WiFi drivers of the Linux kernel^{[65]} and the regulatory domain sections.^{[66]}
 Np
 Another closely related unit is the neper (Np). Like the decibel, the neper is a unit of level.^{[3]}
Fractions
Attenuation constants, in fields such as optical fiber communication and radio propagation path loss, are often expressed as a fraction or ratio to distance of transmission. dB/m represents decibel per meter, dB/mi represents decibel per mile, for example. These quantities are to be manipulated obeying the rules of dimensional analysis, e.g., a 100meter run with a 3.5 dB/km fiber yields a loss of 0.35 dB = 3.5 dB/km × 0.1 km.
See also
 Apparent magnitude
 Cent (music)
 dB drag racing
 Decade (log scale)
 Loudness
 Onethird octave § Base 10
 Phon
 Richter magnitude scale
 Sone
 pH
References
 ^ ^{a} ^{b} ^{c} Utilities : V_{RMS} / dBm / dBu / dBV calculator, Analog Devices, retrieved 20160916
 ^ IEEE Standard 100: a dictionary of IEEE standards and terms (7th ed.). New York: The Institute of Electrical and Electronics Engineering. 2000. p. 288. ISBN 9780738126012.
 ^ ^{a} ^{b} ^{c} "ISO 800003:2006". International Organization for Standardization. Retrieved 20 July 2013.
 ^ Johnson, Kenneth Simonds (1944). Transmission Circuits for Telephonic Communication: Methods of analysis and design. New York: D. Van Nostrand Co. p. 10.
 ^ Davis, Don; Davis, Carolyn (1997). Sound system engineering (2nd ed.). Focal Press. p. 35. ISBN 9780240803050.
 ^ Hartley, R. V. L. (December 1928). "'TU' becomes 'Decibel'". Bell Laboratories Record. AT&T. 7 (4): 137–139.
 ^ Martin, W. H. (January 1929). "DeciBel—The New Name for the Transmission Unit". Bell System Technical Journal. 8 (1).
 ^ 100 Years of Telephone Switching, p. 276, at Google Books, Robert J. Chapuis, Amos E. Joel, 2003
 ^ Harrison, William H. (1931). "Standards for Transmission of Speech". Standards Yearbook. National Bureau of Standards, U. S. Govt. Printing Office. 119.
 ^ Horton, J. W. (1954). "The bewildering decibel". Electrical Engineering. 73 (6): 550–555. doi:10.1109/EE.1954.6438830.
 ^ "Meeting minutes" (PDF). Consultative Committee for Units. Section 3.
 ^ ^{a} ^{b} "Letter symbols to be used in electrical technology". International Electrotechnical Commission. 19 July 2002. Part 3: Logarithmic and related quantities, and their units. IEC 600273, Ed. 3.0.
 ^ ^{a} ^{b} Thompson, A. and Taylor, B. N. sec 8.7, "Logarithmic quantities and units: level, neper, bel", Guide for the Use of the International System of Units (SI) 2008 Edition, NIST Special Publication 811, 2nd printing (November 2008), SP811 PDF
 ^ "Letter symbols to be used in electrical technology". International Standard CEIIEC 273. International Electrotechnical Commission. Part 3: Logarithmic quantities and units.
 ^ Mark, James E. (2007). Physical Properties of Polymers Handbook. Springer. p. 1025.
[…] the decibel represents a reduction in power of 1.258 times […]
 ^ Yost, William (1985). Fundamentals of Hearing: An Introduction (Second ed.). Holt, Rinehart and Winston. p. 206. ISBN 9780127726908.
[…] a pressure ratio of 1.122 equals + 1.0 dB […]
 ^ Fedor Mitschke, Fiber Optics: Physics and Technology, Springer, 2010 ISBN 3642037038.
 ^ Pozar, David M. (2005). Microwave Engineering (3rd ed.). Wiley. p. 63. ISBN 9780471448785.
 ^ I M Mills; B N Taylor; A J Thor (2001), "Definitions of the units radian, neper, bel and decibel", Metrologia, 38 (4): 353, doi:10.1088/00261394/38/4/8
 ^ ^{a} ^{b} R. Hickling (1999), Noise Control and SI Units, J Acoust Soc Am 106, 3048
 ^ Fiber Optics. Springer. 2010.
 ^ R. J. Peters, Acoustics and Noise Control, Routledge, November 12, 2013, 400 pages, p. 13
 ^ Nicholas P. Cheremisinoff (1996) Noise Control in Industry: A Practical Guide, Elsevier, 203 pp, p. 7
 ^ Andrew Clennel Palmer (2008), Dimensional Analysis and Intelligent Experimentation, World Scientific, 154 pp, p.13
 ^ J. C. Gibbings, Dimensional Analysis, p.37, Springer, 2011 ISBN 1849963177.
 ^ Sensation and Perception, p. 268, at Google Books
 ^ Introduction to Understandable Physics, Volume 2, p. SA19PA9, at Google Books
 ^ Visual Perception: Physiology, Psychology, and Ecology, p. 356, at Google Books
 ^ Exercise Psychology, p. 407, at Google Books
 ^ Foundations of Perception, p. 83, at Google Books
 ^ Fitting The Task To The Human, p. 304, at Google Books
 ^ ISO 1683:2015
 ^ C. S. Clay (1999), Underwater sound transmission and SI units, J Acoust Soc Am 106, 3047
 ^ NoiseInduced Hearing Loss, National Institute on Deafness and Other Communications Disorders, 2008, archived from the original on 9 May 2016
 ^ Chomycz, Bob (2000). Fiber optic installer's field manual. McGrawHill Professional. pp. 123–126. ISBN 9780071356046.
 ^ Stephen J. Sangwine and Robin E. N. Horne (1998). The Colour Image Processing Handbook. Springer. pp. 127–130. ISBN 9780412806209.
 ^ Francis T. S. Yu and Xiangyang Yang (1997). Introduction to optical engineering. Cambridge University Press. pp. 102–103. ISBN 9780521574938.
 ^ Junichi Nakamura (2006). "Basics of Image Sensors". In Junichi Nakamura. Image sensors and signal processing for digital still cameras. CRC Press. pp. 79–83. ISBN 9780849335457.
 ^ Winer, Ethan (2013). The Audio Expert: Everything You Need to Know About Audio. Focal Press. p. 107. ISBN 9780240821009.
 ^ stason.org, Stas Bekman: stas (at). "3.3  What is the difference between dBv, dBu, dBV, dBm, dB SPL, and plain old dB? Why not just use regular voltage and power measurements?". stason.org.
 ^ Rupert Neve, Creation of the dBu standard level reference
 ^ deltamedia.com. "DB or Not DB". Deltamedia.com. Retrieved 20130916.
 ^ The IEEE Standard Dictionary of Electrical and Electronics terms (6th ed.). IEEE. 1996 [1941]. ISBN 9781559378338.
 ^ Jay Rose (2002). Audio postproduction for digital video. Focal Press. p. 25. ISBN 9781578201167.
 ^ Morfey, C. L. (2001). Dictionary of Acoustics. Academic Press, San Diego.
 ^ ANSI, S1.419823 Specification for Sound Level Meters, 2.3 Sound Level, p. 23.
 ^ Zimmer, Walter MX, Mark P. Johnson, Peter T. Madsen, and Peter L. Tyack. "Echolocation clicks of freeranging Cuvier’s beaked whales (Ziphius cavirostris)." The Journal of the Acoustical Society of America 117, no. 6 (2005): 3919–3927.
 ^ http://oto2.wustl.edu/cochlea/wt4.html
 ^ Bigelow, Stephen (2001). Understanding Telephone Electronics. Newnes. p. 16. ISBN 9780750671750.
 ^ Tharr, D. (1998). Case Studies: Transient Sounds Through Communication Headsets. Applied Occupational and Environmental Hygiene, 13(10), 691–697.
 ^ ITUR BS.1770
 ^ "Glossary: D's". National Weather Service. Retrieved 20130425.
 ^ "Radar FAQ from WSI". Archived from the original on 18 May 2008. Retrieved 20080318.
 ^ "Definition at Everything2". Retrieved 20080806.
 ^ Carr, Joseph (2002). RF Components and Circuits. Newnes. pp. 45–46. ISBN 9780750648448.
 ^ "The dBµ vs. dBu Mystery: Signal Strength vs. Field Strength?". radiotimetraveller.blogspot.com. Retrieved 13 October 2016.
 ^ Chand, N., Magill, P. D., Swaminathan, S. V., & Daugherty, T. H. (1999). Delivery of digital video and other multimedia services (> 1 Gb/s bandwidth) in passband above the 155 Mb/s baseband services on a FTTx full service access network. Journal of lightwave technology, 17(12), 2449–2460.
 ^ David Adamy. EW 102: A Second Course in Electronic Warfare. Retrieved 20130916.
 ^ ITUT Rec. G.100.1 The use of the decibel and of relative levels in speechband telecommunications https://www.itu.int/rec/dologin_pub.asp?lang=e&id=TRECG.100.1201506I!!PDFE&type=items
 ^ dBrnC is defined on page 230 in "Engineering and Operations in the Bell System," (2ed), R.F. Rey (technical editor), copyright 1983, AT&T Bell Laboratories, Murray Hill, NJ, ISBN 0932764045
 ^ K. N. Raja Rao (20130131). Satellite Communication: Concepts And Applications. Retrieved 20130916.
 ^ Ali Akbar Arabi. Comprehensive Glossary of Telecom Abbreviations and Acronyms. Retrieved 20130916.
 ^ Mark E. Long. The Digital Satellite TV Handbook. Retrieved 20130916.
 ^ Mac E. Van Valkenburg (20011019). Reference Data for Engineers: Radio, Electronics, Computers and Communications. Retrieved 20130916.
 ^ "en:users:documentation:iw [Linux Wireless]". wireless.kernel.org.
 ^ "Is your WiFi AP Missing Channels 12 & 13?". wordpress.com. 16 May 2013.
Further reading
 Tuffentsammer, Karl (1956). "Das Dezilog, eine Brücke zwischen Logarithmen, Dezibel, Neper und Normzahlen" [The decilog, a bridge between logarithms, decibel, neper and preferred numbers]. VDIZeitschrift (in German). 98: 267–274.
 Paulin, Eugen (20070901). Logarithmen, Normzahlen, Dezibel, Neper, Phon  natürlich verwandt! [Logarithms, preferred numbers, decibel, neper, phon  naturally related!] (PDF) (in German). Archived (PDF) from the original on 20161218. Retrieved 20161218.
External links
 What is a decibel? With sound files and animations
 Conversion of sound level units: dBSPL or dBA to sound pressure p and sound intensity J
 OSHA Regulations on Occupational Noise Exposure
 Working with Decibels (RF signal and field strengths)